Filtern
Erscheinungsjahr
- 2009 (116) (entfernen)
Dokumenttyp
- Dissertation (116) (entfernen)
Sprache
- Englisch (116) (entfernen)
Volltext vorhanden
- ja (116)
Gehört zur Bibliographie
- nein (116) (entfernen)
Schlagworte
- Wirkstoff-Rezeptor-Bindung (4)
- Licht-Sammel-Komplex (3)
- Ligand <Biochemie> (3)
- Membranproteine (3)
- Theoretische Physik (3)
- Algebraische Geometrie (2)
- Biochemie (2)
- Crystallography (2)
- FT-IR-Spektroskopie (2)
- Gestaltwahrnehmung (2)
Institut
- Biochemie und Chemie (33)
- Physik (24)
- Biowissenschaften (19)
- Geowissenschaften (6)
- Medizin (6)
- Pharmazie (5)
- Mathematik (4)
- Psychologie (4)
- Informatik (3)
- Frankfurt Institute for Advanced Studies (FIAS) (2)
Drought and salt stress are the major constraint to increase yield in chickpea (Cicer arietinum). Improving drought and high-salinity tolerance is therefore of outmost importance for breeding. However, the complexity of these traits allowed only marginal progress. A solution to the current stagnation is expected from innovative molecular tools such as transcriptome analyses providing insight into stress-related gene activity, which combined with molecular markers and expression (e)QTL mapping, may accelerate knowledge-based breeding. SuperSAGE, an improved version of the serial analysis of gene expression (SAGE) technique, generating genome-wide, high-quality transcription profiles from any eukaryote, has been employed in the present study. The method produces 26bp long fragments (26bp tags) from defined positions in cDNAs, providing sufficient sequence information to unambiguously characterize the mRNAs. Further, SuperSAGE tags may be immediately used to produce microarrays and probes for real-time-PCR, thereby overcoming the lack of genomic tools in non-model organisms.
Many questions regarding gastropod phylogeny have not yet been answered like the molecular confirmation of the Heterobranchia concept based on morphological studies from Haszprunar (1985a; 1988). This taxon contains the “Lower Heterobranchia” with several “primitive” or “basal” members) and the Euthyneura (with the Opisthobranchia and Pulmonata). Phylogenetic relationships of subgroups within the Heterobranchia have not been satisfactorily resolved and monophyly of some taxa within the Heterobranchia (e.g. Opisthobranchia) is questionable. Moreover, most of the “Lower Heterobranchia” have not been included in former molecular studies. In order to resolve phylogenetic relationships within the Heterobranchia, I pursued a molecular systematic approach by sequencing and analysing a variety of genetic markers (including nuclear 28S rDNA + 18S rDNA and mitochondrial 16S rDNA + COI sequences). Maximum likelihood as well as Bayesian inference methods were used for phylogenetic reconstruction. The data were investigated a priori to tree reconstruction in order to find the most appropriate dataset for reconstructing heterobranch phylogeny. A variety of statistical tests (like Chi-Square-Test or Relative-Rate-Test) were applied and the substitution saturation was measured. The Relative-Rate-Test revealed the highest evolution rates within the “Lower Heterobranchia” (Omalogyra sp., Omalogyra fusca, Murchisonella sp., Ebala sp. and Architectonica perspectiva) and Opisthobranchia (Hyalocylis striata). Furthermore, many of the nucleotide positions show a high degree of substitution saturation. Additionally, bipartitions (splits) in the alignment were examined and visualized by split network analyses to estimate data quality. A high level of conflict indicated by many parallel edges of the same lengths could be observed in the neighbournet graphs. Moreover, several taxa with long terminal branches could be identified in all three datasets belonging to the Vetigastropoda, Caenogastropoda, “Lower Heterobranchia” or Opisthobranchia (Nudipleura). All phylogenetic analyses revealed a monophyletic Heterobranchia. Within the Heterobranchia several well supported clades could be resolved. However, the traditional classification based on morphological data could not be confirmed due to paraphyletic Euthyneura (because of the inclusion of the Pyramidellidae and Glacidorboidea) as well as paraphyletic Pulmonata and polyphyletic Opisthobranchia. Based on the phylogenetic inferred evolutionary trends regarding habitat colonisation or character complexes could be deduced. A case study was conducted in order to estimate divergence ages using a “relaxed” molecular clock approach with fossils as minimum age constraints. However, due to large 95% confidence intervals a precise dating of the nodes was not possible. Hence, the results are considered as preliminary. To test the plausibility of the newly obtained hypotheses, the results were evaluated a posteriori using a hypothesis test and secondary structures of the complete 18S rRNA and 28S rRNA. Secondary structure motifs were found within domain 43 and E23 2 &5 of the 18S rRNA as well as within domain E11 and G5_1 of the 28S rRNA, which contain phylogenetic signals to support various groups within the Heterobranchia. In addition, taxon specific motifs were found separating the Vetigastropoda from the Caenogastropoda and Heterobranchia, indicating a possible application of the secondary structure of 18S rRNA and 28S rRNA to reveal phylogenetic relationships at higher taxonomic levels such as Gastropoda or even Mollusca. The utility of the newly invented software RNAsalsa for the reconstruction of secondary structures was tested. The obtained structures were used to adjust evolutionary models specific to rRNA stem (paired basepairs) and loop (unpaired basepairs) regions with the intention of improving phylogenetic results. This approach proved unsuccessful. This molecular phylogenetic investigation provides the most comprehensive molecular study of Heterobranchia relationships to date. Substantial insights into the evolution and phylogeny of this enigmatic taxon have been gained.
In this work the preparation of organic donor-acceptor thin films was studied. A chamber for organic molecular beam deposition was designed and integrated into an existing deposition system for metallic thin films. Furthermore, the deposition system was extended by a load-lock with integrated bake-out function, a chamber for the deposition of metallic contacts via stencil mask technique and a sputtering chamber. For the sublimation of the organic compounds several effusion cells were designed. The evaporation characteristic and the temperature profile within the cells was studied. Additionally, a simulation program was developed, which calculates the evaporation characteristics of different cell types. The following processes were integrated: evaporation of particles, migration on the cell walls and collisions in the gas phase. It is also possible to consider a temperature gradient within the cell. All processes can be studied separately and their relative strength can be varied. To verify the simulation results several evaporation experiments with different cell types were employed. The thickness profile of the prepared thin films was measured position-dependently. The results are in good agreement with the simulation. Furthermore, the simulation program was extended to the field of electron beam induced deposition (EBID). The second part of this work deals with the preparation and characterization of organic thin films. The focus hereby lies on the charge transfer salt (BEDT-TTF)(TCNQ), which has three known structure variants. Thin films were prepared by different methods of co-evaporation and were studied with optical microscopy, X-ray diffraction and energy dispersive X-ray spectroscopy (EDX).The formation of the monoclinic phase of (BEDT-TTF)(TCNQ) could be shown. As a last part tunnel structures were prepared as first thin film devices and measured in a He4 cryostat.
Induced charge computation
(2009)
One of the main aspects of statistical mechanics is that the properties of a thermodynamics state point do not depend on the choice of the statistical ensemble. It breaks down for small systems e.g. single molecules. Hence, the choice of the statistical ensemble is crucial for the interpretation of single molecule experiments, where the outcome of measurements depends on which variables or control parameters, are held fixed and which ones are allowed to fluctuate. Following this principle, this thesis investigates the thermodynamics of a single polymer pulling experiments within two different statistical ensembles. The scaling of the conjugate chain ensembles, the fixed end-to-end vector (Helmholtz) and the fixed applied force (Gibbs), are studied in depth. This thesis further investigates the ensemble equivalence for different force regimes and polymer-chain contour lengths. Using coarse-grained molecular dynamic simulations, i.e. Langevin dynamics, the simulations were found to complement the theoretical predictions for the scaling of ensemble difference of Gaussian chains in different force-regimes, giving special attention to the zero force regime. After constructing Helmholtz and Gibbs conjugate ensembles for a Gaussian chain, two different data sets of thermodynamic states on the force-extension plane, i.e. force-extension curves, were generated. The ensemble difference is computed for different polymer-chain lengths by using force-extension curves. The scaling of the ensemble difference versus relative polymer-chain length under different force regimes has been derived from the simulation data and compared to theoretical predictions. The results demonstrate that the Gaussian chain in the zero force limit generates nonequivalent ensembles, regardless of its equilibrium bond length and polymer-chain contour length. Moreover, if polymers are charged in confinement, coarse-graining is problematic, owing to dielectric interfaces. Hence, the effect of dielectric interfaces must be taken into account when describing physical systems such as ionic channels or biopolymers inside nanopores. It is shown that the effect of dielectrics is crucial for the dynamics of a biopolymer or an ion inside a nanopore. In the simulations, the feasibility of an efficient and accurate computation of electrostatic interactions in the presence of an arbitrarily shaped dielectric domain is challenging. Several solutions for this problem have been previously proposed in the literature such as a density functional approach, or transforming problem at hand into an algebraic problem ( Induced Charge Computation (ICC) ) and boundary element methods. Even though the essential concept is the same, which is to replace the dielectric interface with a polarization charge density, these approaches have been analyzed and the ICC algorithm has been implemented. A new superior boundary element method has been devised utilizing the force computation via the Particle-Particle Particle-Mesh (P3M) method for periodic geometries (ICCP3M). This method has been compared to the ICC algorithm, the algebraic solutions, and to density functional approaches. Extensive numerical tests against analytically tractable geometries have confirmed the correctness and applicability of developed and implemented algorithms, demonstrating that the ICCP3M is the fastest and the most versatile algorithm. Further optimization issues are also discussed in obtaining accurate induced charge densities. The potential of mean force (PMF) of DNA modelled on a coarsed-grain level inside a nanopore is investigated with and without the inclusion of dielectric effects. Despite the simplicity of the model, the dramatic effect of dielectric inclusions is clearly seen in the observed force profile.
Global warming is expected to be associated with diverse changes in freshwater habitats in north-western Europe. Increasing evaporation, lower oxygen concentration due to increased water temperature and changes in precipitation pattern are likely to affect the survival ratio and reproduction rate of freshwater gastropods (Pulmonata, Basommatophora). This work is a comprehensive analyse of the climatic factors influencing their ranges both in the past and in the near future. A macroecological approach showed that for a great proportion of genera the ranges were projected to contract by 2080, even if unlimited dispersal was assumed. The forecasted warming in the cooler northern ranges predicted the emergence of new suitable areas, but also reduced drastically the available habitat in the southern part of the studied region. In order to better understand the ranges dynamics in the past and the post glacial colonisation patterns, an approach combining ecological niche modelling and phylogeography was used for two model species, Radix balthica and Ancylus fluviatilis. Phylogeographic model selection on a COI mtDNA dataset confirmed that R. balthica most likely spread from two central European disjunct refuges after the last glacial maximum. The phylogeographic analysis of A. fluviatilis, using 16S and COI mtDNA datasets, also inferred central European refugia. The absence of niche conservatism (adaptive potential) inferred for A. fluviatilis puts a cautionary note on the use of climate envelope models to predict the future ranges of this species. However, the other model species exhibited strong niche conservatism, which allow putting confidence into such predictions. A profound faunal shift will take place in Central Europe within the next century, either permitting the establishment of species currently living south of the studied region or the proliferation of organisms relying on the same food resources. This study points out the need for further investigations on the dispersal modes of freshwaters snails, since the future range size of the species depend on their ability to establish in newly available habitats. Likewise, the mixed mating system of these organisms gives them the possibility to fund a new population from a single individual. It will probably affect the colonisation success and needs further investigation.
Lentiviral vectors mediate gene transfer into dividing and most non-dividing cells. Thereby, they stably integrate the transgene into the host cell genome. For this reason, lentiviral vectors are a promising tool for gene therapy. However, safety and efficiency of lentiviral mediated gene transfer still needs to be optimised. Ideally, cell entry should be restricted to the cell population relevant for a particular therapeutic application. Furthermore, lentiviral vectors able to transduce quiescent lymphocytes are desirable. Although many approaches were followed to engineer retroviral envelope proteins, an effective and universally applicable system for retargeting of lentiviral cell entry is still not available. Just before the experimental work of this thesis was started, retargeting of measles virus (MV) cell entry was achieved. This virus has two types of envelope glycoproteins, the hemagglutinin (H) protein responsible for receptor recognition and the fusion (F) protein mediating membrane fusion. For retargeting, the H protein was mutated in its interaction sites for the native MV receptors and a ligand or a single-chain antibody (scAb) was fused to its ectodomain. It was hypothesised that the retargeting system of MV can be transferred to lentiviral vectors by pseudotyping human immunodeficiency virus-1 (HIV-1) derived vector particles with the MV glycoproteins. As the unmodified MV glycoproteins did not pseudotype HIV vectors, two F and 15 H protein variants carrying stepwise truncations or amino acid (aa) exchanges in their cytoplasmic tails were screened for their ability to form MV-HIV pseudotypes. The combinations Hcd18/Fcd30, Hcd19/Fcd30 and Hcd24+4A/Fcd30 led to most efficient pseudotype formation with titers above 10exp6 transducing units /ml, using concentrated particles. The F cytoplasmic tail was truncated by 30 aa and the H cytoplasmic tail was truncated by 18, 19 or 24 residues with four added alanines after the start methionine in the latter case. Western blot analysis indicated that particle incorporation of the MV glycoproteins was enhanced upon truncation of their cytoplasmic tails. With the MV-HIV vectors high titers on different cell lines expressing one or both MV receptors were obtained, whereas MV receptor-negative cells remained untransduced. Titers were enhanced using an optimal H to F plasmid ratio (1:7) during vector particle production. Based on the described pseudotyping with the MV glycoprotein variants, HIV vectors retargeted to the epidermal growth factor receptor (EGFR) or the B cell surface marker CD20 were generated. For the production of the retargeted vectors MVaEGFR-HIV and MVaCD20-HIV, Fcd30 together with a native receptor blind Hcd18 protein, displaying at its ectodomain either the ligand EGF or a scAb directed against CD20 were used. With these vectors, gene transfer into target receptor-positive cells was several orders of magnitude more efficient than into control cells. The almost complete absence of background transduction of non-target cells was e.g. demonstrated in mixed cell populations, where the CD20-targeting vector selectively eliminated CD20-positive cells upon suicide gene transfer. Remarkably, transduction of activated primary human CD20-positive B cells was much more efficient with the MVaCD20-HIV vector than with the standard pseudotype vector VSV-G-HIV. Even more surprisingly, MVaCD20-HIV vectors were able to transduce quiescent primary human B cells, which until then had been resistant towards lentiviral gene transfer. The most critical step during the production of MV-HIV pseudotypes was the identification of H cytoplasmic tail mutants that allowed pseudotyping while retaining the fusion helper function. In contrast to previously inefficient targeting strategies, the reason for the success of this novel targeting system must be based on the separation of the receptor recognition and fusion functions onto two different proteins. Furthermore, with the CD20-targeting vector transduction of quiescent B cells was demonstrated for the first time. Own data and literature data suggest that CD20 binding and hyper-cross-linking by the vector particles results in calcium influx and thus activation of quiescent B cells. Alternatively this feature may be based on a residual binding activity of the MV glycoproteins to the native MV receptors that is insufficient for entry but induces cytoskeleton rearrangements dissolving the post-entry block of HIV vectors. Hence, in this thesis efficient retargeting of lentiviral vectors and transduction of quiescent cells was combined. This novel targeting strategy should be easily adaptable to many other target molecules by extending the modified MV H protein with appropriate specific domains or scAbs. It should now be possible to tailor lentiviral vectors for highly selective gene transfer into any desired target cell population with an unprecedented degree of efficiency.
Neutron stars are very dense objects. One teaspoon of their material would have a mass of five billion tons. Their gravitational force is so strong that if an object were to fall from just one meter high it would hit the surface of the respective neutron star at two thousand kilometers per second. In such dense bodies, different particles from the ones present in atomic nuclei, the nucleons, can exist. These particles can be hyperons, that contain non-zero strangeness, or broader resonances. There can also be different states of matter inside neutron stars, such as meson condensates and if the density is height enough to deconfine the nucleons, quark matter. As new degrees of freedom appear in the system, different aspects of matter have to be taken into account. The most important of them being the restoration of the chiral symmetry. This symmetry is spontaneously broken, which is a fact related to the presence of a condensate of scalar quark-antiquark pairs, that for this reason is called chiral condensate. This condensate is present at low densities and even in vacuum. It is important to remember at this point that the modern concept of vacuum is far away from emptiness. It is full of virtual particles that are constantly created and annihilated, being their existence allowed by the uncertainty principle. At very high temperature/density, when the composite particles are dissolved into constituents, the chiral consensate vanishes and the chiral symmetry is restored. To explain how and when chiral symmetry is restored in neutron stars we use a model called non-linear sigma model. This is an effective quantum relativistic model that was developed in order to describe systems of hadrons interacting via meson exchange. The model was constructed from symmetry relations, which allow it to be chiral invariant. The first consequence of this invariance is that there are no bare mass terms in the lagrangian density, causing all, or most of the particles masses to come from the interactions with the medium. There are still other interesting features in neutron stars that cannot be found anywhere else in nature. One of them is the high isospin asymmetry. In a normal nucleus, the amount of protons and neutrons is more or less the same. In a neutron star the amount of neutrons is much higher than the protons. The resulting extra energy (called Fermi energy) increases the energy of the system, allowing the star to support more mass against gravitational collapse. As a consequence of that in early stages of the neutron star evolution, when there are still many trapped neutrinos, the proton fraction is higher than in later stages and consequently the maximum mass that the star can support against gravity is smaller. This, between many other features, shows how the microscopic phenomena of the star can reflect into the macroscopic properties. Another important property of neutron stars is charge neutrality. It is a required assumption for stability in neutron stars, but there are others. One example is chemical equilibrium. It means that the number of particles from each kind is not conserved, but they are created and annihilated through specific reactions that happen at the same rate in both directions. Although to calculate microscopic physics of neutron stars the space-time of special relativity, the Minkowski space, can be used, this is not true for the global properties of the star. In this case general relativity has to be used. The solution of Einstein's equations simplified to static, spherical and isotropic stars correspond to the configurations in which the star is in hydrostatic equilibrium. That means that the internal pressure, coming mainly from the Fermi energy of the neutrons, balances the gravity avoiding the collapse. When rotation is included the star becomes more stable, and consequently, can be more massive. The movement also makes it non-spherical, what requires the metric of the star to also be a function of the polar coordinate. Another important feature that has to be taken into account is the dragging of the local inertial frame. It generates centrifugal forces that are not originated in interactions with other bodies, but from the non-rotation of the frame of reference within which observations are made. These modifications are introduced through the Hartle's approximation that solves the problem by applying perturbation theory. In the mean field approximation, the couplings as well as the parameters of the non-linear sigma model are calibrated to reproduce massive neutron stars. The introduction of new degrees of freedom decreases the maximum mass allowed for the neutron star, as they soften the equation of state. In practice, the only baryons present in the star besides the nucleons are the Lambda and Sigma-, in the case in which the baryon octet is included, and Lambda and Delta-,0,+,++, in the case in which the baryon decuplet is included. The leptons are included to ensure charge neutrality. We choose to proceed our calculations including the baryon octet but not the decuplet, in order to avoid uncertainties in the couplings. The couplings of the hyperons were fitted to the depth of their potentials in nuclei. In this case the chiral symmetry restoration can be observed through the behavior of the related order parameter. The symmetry begins to be restored inside neutron stars and the transition is a smooth crossover. Different stages of the neutron star cooling are reproduced taking into account trapped neutrinos, finite temperature and entropy. Finite-temperature calculations include the heat bath of hadronic quasiparticles within the grand canonical potential of the system. Different schemes are considered, with constant temperature, metric dependent temperature and constant entropy. The neutrino chemical potential is introduced by fixing the lepton number in the system, that also controls the amount of electrons and protons (for charge neutrality). The balance between these two features is delicate and influenced mainly by the baryon number conservation. Isolated stars have a fixed number of baryons, which creates a link between different stages of the cooling. The maximum masses allowed in each stage of the cooling process, the one with high entropy and trapped neutrinos, the deleptonized one with high entropy, and the cold one in beta equilibrium. The cooling process is also influenced by constraints related to the rotation of the star. When rotation is included the star becomes more stable, and consequently, can be more massive. The movement also deforms it, requiring the metric of the star to include modifications that are introduced through the use of perturbation theory. The analysis of the first stages of the neutron star, when it is called proto-neutron star, gives certain constraints on the possible rotation frequencies in the colder stages. Instability windows are calculated in which the star can be stable during certain stages but collapses into black holes during the cooling process. In the last part of the work the hadronic SU(3) model is extended to include quark degrees of freedom. A new effective potential to the order parameter for deconfinement, the Polyakov loop, makes the connection between the physics at low chemical potential and hight temperature of the QCD phase diagram with the height chemical potential and low temperature part. This is done through the introduction of a chemical potential dependency on the already temperature dependent potential. Analyzing the effect of both order parameters, the chiral condensate and the Polyakov loop, we can drawn a phase diagram for symmetric as well as for star matter. The diagram contains a crossover region as well as a first order phase transition line. The new couplings and parameters of the model are chosen mainly to fit lattice QCD, including the position of the critical point. Finally, this matter containing different degrees of freedom (depending on which phase of the diagram we are) is used to calculate hybrid star properties.
Das libor Markt Modell (LMM) ist seit seiner Entwicklung in den Veröffentlichungen von Brace, Gatarek, Musiela (1997), einerseits, und unabhängig von diesen von Miltersen, Sandmann, Sondermann (1997), andererseits, zu dem anerkanntesten Instrument zur Modellierung der Zinsstruktur und der damit verbundenen Preisfindung für relevante Finanzderivate geworden. libor steht dabei für London Inter-Bank Offered Rate, ein täglich in London fixierter Referenz-Zins für kurzfristige Anlagen. Drei- oder sechsmonatige Laufzeiten sind in Verbindung mit dem LMM üblich. Die Forschung zur Verbesserung dieses Modells hat in den letzten Jahren an Zuwachs gewonnen. Beim Versuch den Fehler der Anpassung an die täglich beobachteten Preise von Zinsoptionen wie Caps und Swaptions zu verringern, erhält man in der Folge auch genauere Bewertungen für andere, exotischere, Derivate. Die zugrunde liegende und zentrale Idee des LMM besteht darin, die Forward (Termin) Zinsen direkt als primären (Vektor) Prozess mehrerer libor Sätze zu betrachten und diese simultan zu modellieren, anstatt sie nur herzuleiten aus einem übergeordneten, unendlich dimensionalen Forward Zinsprozess, wie im zeitlich früher entwickelten Heath-Jarrow-Morton Modell. Das überzeugendste Argument für diese Diskretisierung ist, dass die libor Sätze direkt im Markt beobachtbar sind und ihre Volatilitäten auf eine natürliche Weise in Beziehung gebracht werden können zu bereits liquide gehandelten Produkten, eben jenen Caps und Swaptions. Dennoch beinhaltet das Modell eine gravierende Insuffizienz, indem es keine Krümmung der Volatilitätsoberfläche, im Hinblick auf Optionen mit verschiedenen Basiszinsen, abbildet. Wie im einfachen eindimensionalen Black-Scholes Modell prägen sich auch hier die Ungenauigkeiten der Verteilung in fehlenden heavy tails deutlich aus. Smile und Skew Effekte sind erkennbar. Im klassischen liborMarkt Modell wird in Richtung der Basiszinsdimension nur eine affine Struktur erzeugt, welche bestenfalls als Approximation für die erwünschte Oberfläche dienen kann. Die beobachteten Verzerrungen führen naturgemäss zu einer ungenauen Abbildung der Realität und fehlerhaften Reproduktion der Preise in Regionen, die ein wenig entfernt vom Bereich am Geld liegen. Derartig ungewollte Dissonanzen in Gewinn und Verlustzahlen führten z.B. in 1998 zu gravierenden Verlusten im Zinsderivateportfolio der heutigen Royal Bank of Scotland. ...
The NADH:ubiquinone oxidoreductase (complex I) is a large membrane bound protein complex coupling the redox reaction of NADH oxidation and quinone reduction to vectorial proton translocation across bioenergetic membranes. The mechanism of proton pumping is still unknown; it seems however that the reduction of quinone induces conformational changes which drive proton uptake from one side and release at the other side of the membrane. In this study the proposed quinone and inhibitor binding pocket located at the interface of the 49-kDa and PSST subunits was explored by a large number of point mutations introduced into complex I from the strictly aerobic yeast Yarrowia lipolytica. Point mutations were systematically chosen based on the crystal structure of the hydrophilic domain of complex I from Thermus thermophilus. In total, the properties of 94 mutants at 39 positions which completely cover the lining of the large putative quinone and inhibitor binding cavity are described and discussed here. A structure/function analysis allowed the identification of functional domains within the large putative quinone binding cavity. A possible quinone access path ranging from the N-terminal beta-sheet of the 49-kDa subunit into the pocket to tyrosine 144 could be defined, since all exchanges introduced here, caused an almost complete loss of complex I activity. A region located deeper in the proposed quinone binding pocket is apparently not important for complex I activity. In contrast, all exchanges of tyrosine 144, even the very conservative mutant Y144F, essentially abolished dNADH:DBQ oxidoreductase activity of complex I. However, with higher concentrations of Q1 or Q2 the dNADH:Q oxidoreductase activity was largely restored in the mutants with the more conservative exchanges. Proton pumping experiments showed that this activity was also coupled to proton translocation, indicating that these quinones were reduced at the physiological site. However, the apparent Km values for Q1 or Q2 were drastically increased, clearly demonstrating that tyrosine 144 is central for quinone binding and reduction. These results further prove that the enzymatically relevant quinone binding site of complex I is located at the interface of the 49-kDa and PSST subunits. The quinone binding pocket is thought to comprise the binding sites for a plethora of specific complex I inhibitors that are usually grouped into three classes. The large array of mutants targeting the quinone binding cavity was examined with a representative of each inhibitor class. Many mutants conferring resistance were identified which, depending on the inhibitor tested, clustered in well defined and partially overlapping regions of the large putative quinone and inhibitor binding cavity. Mutants with effects on type A (DQA) and type B (rotenone) inhibitors were found in a subdomain corresponding to the former [NiFe] site in homologous hydrogenases, whereby the type A inhibitor DQA seems to bind deeper in this domain. Mutants with effects on the type C inhibitor (C12E8) were found in a narrow crevice. Exchanging more exposed residues at the border of these well defined domains affected all three inhibitor types. Therefore, the results as a whole provide further support for the concept that different inhibitor classes bind to different but partially overlapping binding sites within a single large quinone binding pocket. In addition, they also indicate the approximate location of the binding sites within the structure of the large quinone and inhibitor binding cavity at the interface of the 49 kDa and the PSST subunit. It has been proposed earlier that the highly conserved HRGXE-motif in the 49-kDa subunit forms a part of the quinone binding site of complex I. Mutagenesis of the HRGXE-motif, revealed that these residues are rather critical for complex I assembly and seem to have an important structural role. The question why iron-sulfur cluster N1a is not detectable by EPR in many models organisms is not solved yet. Introducing polar and positively charged amino acid residues close to this cluster in order to increase its midpoint potential did not result in the appearance of the cluster N1a EPR signal in mitochondrial membranes from the mutants. Clearly, further research will be necessary to gain insights to the function of this iron-sulfur cluster in complex I. In an additional project, a new and simple in vivo screen for complex I deficiency in Y. lipolytica was developed and optimized. This assay probes for defects in complex I assembly and stability, oxidoreductase activity and also proton pumping activity by complex I. Most importantly, this assay is applicable to all Y. lipolytica strains and could be used to identify loss-of-function mutants, gain-of-functions mutants (i.e. resistance towards complex I inhibitors) and revertants due to mutations in both nuclear and mitochondrially encoded genes of complex I subunits.
The light-harvesting complex of photosystem II (LHC-II) is the major antenna complex in plant photosynthesis. It accounts for roughly 30% of the total protein in plant chloroplasts, which makes it arguably the most abundant membrane protein on Earth, and binds about half of plant chlorophyll (Chl). The complex assembles as a trimer in the thylakoid membrane and binds a total of 54 pigment molecules, including 24 Chl a, 18 Chl b, 6 lutein (Lut), 3 neoxanthin (Neo) and 3 violaxanthin (Vio). LHC-II has five key roles in plant photosynthesis. It: (1) harvests sunlight and transmits excitation energy to the reaction centres of photosystems II and I, (2) regulates the amount of excitation energy reaching each of the two photosystems, (3) has a structural role in the architecture of the photosynthetic supercomplexes, (4) contributes to the tight appression of thylakoid membranes in chloroplast grana, and (5) protects the photosynthetic apparatus from photo damage by non photochemical quenching (NPQ). A major fraction of NPQ is accounted for its energy-dependent component qE. Despite being critical for plant survival and having been studied for decades, the exact details of how excess absorbed light energy is dissipated under qE conditions remain enigmatic. Today it is accepted that qE is regulated by the magnitude of the pH gradient (ΔpH) across the thylakoid membrane. It is also well documented that the drop in pH in the thylakoid lumen during high-light conditions activates the enzyme violaxanthin de-epoxidase (VDE), which converts the carotenoid Vio into zeaxanthin (Zea) as part of the xanthophyll cycle. Additionally, studies with Arabidopsis mutants revealed that the photosystem II subunit PsbS is necessary for qE. How these physiological responses switch LHC-II from the active, energy transmitting to the quenched, energy-dissipating state, in which the solar energy is not transmitted to the photosystems but instead dissipated as heat, remains unclear and is the subject of this thesis. From the results obtained during this doctoral work, five main conclusions can be drawn concerning the mechanism of qE: 1. Substitution of Vio by Zea in LHC-II is not sufficient for efficient dissipation of excess excitation energy. 2. Aggregation quenching of LHC-II does not require Vio, Neo nor a specific Chl pair. 3. With one exception, the pigment structure in LHC-II is rigid. 4. The two X-ray structures of LHC-II show the same energy transmitting state of the complex. 5. Crystalline LHC-II resembles the complex in the thylakoid membrane. Models of the aggregation quenching mechanism in vitro and the qE mechanism in vivo are presented as a corollary of this doctoral work. LHC-II aggregation quenching in vitro is attributed to the formation of energy sinks on the periphery of LHC-II through random interaction with other trimers, free pigments or impurities. A similar but unrelated process is proposed to occur in the thylakoid membrane, by which excess excitation energy is dissipated upon specific interaction between LHC-II and a PsbS monomer carrying Zea. At the end of this thesis, an innovative experimental model for the analysis of all key aspects of qE is proposed in order to finally solve the qE enigma, one of the last unresolved problems in photosynthesis research.
In this thesis the first fully integrated Boltzmann+hydrodynamics approach to relativistic heavy ion reactions has been developed. After a short introduction that motivates the study of heavy ion reactions as the tool to get insights about the QCD phase diagram, the most important theoretical approaches to describe the system are reviewed. To model the dynamical evolution of the collective system assuming local thermal equilibrium ideal hydrodynamics seems to be a good tool. Nowadays, the development of either viscous hydrodynamic codes or hybrid approaches is favoured. For the microscopic description of the hadronic as well as the partonic stage of the evolution transport approaches have beeen successfully applied, since they generate the full phse-space dynamics of all the particles. The hadron-string transport approach that this work is based on is the Ultra-relativistic Quantum Molecular Dynamics (UrQMD) approach. It constitutes an effective solution of the relativistic Boltzmann equation and is restricted to binary collisions of the propagated hadrons. Therefore, the Boltzmann equation and the basic assumptions of this model are introduced. Furthermore, predictions for the charged particle multiplicities at LHC energies are made. The next step is the development of a new framework to calculate the baryon number density in a transport approach. Time evolutions of the net baryon number and the quark density have been calculated at AGS, SPS and RHIC energies and the new approach leads to reasonable results over the whole energy range. Studies of phase diagram trajectories using hydrodynamics are performed as a first move into the direction of the development of the hybrid approach. The hybrid approach that has been developed as the main part of this thesis is based on the UrQMD transport approach with an intermediate hydrodynamical evolution for the hot and dense stage of the collision. The initial energy and baryon number density distributions are not smooth and not symmetric in any direction and the initial velocity profiles are non-trivial since they are generated by the non-equilibrium transport approach. The fulll (3+1) dimensional ideal relativistic one fluid dynamics evolution is solved using the SHASTA algorithm. For the present work, three different equations of state have been used, namely a hadron gas equation of state without a QGP phase transition, a chiral EoS and a bag model EoS including a strong first order phase transition. For the freeze-out transition from hydrodynamics to the cascade calculation two different set-ups are employed. Either an in the computational frame isochronous freeze-out or an gradual freeze-out that mimics an iso-eigentime criterion. The particle vectors are generated by Monte Carlo methods according to the Cooper-Frye formula and UrQMD takes care of the final decoupling procedure of the particles. The parameter dependences of the model are investigated and the time evolution of different quantities is explored. The final pion and proton multiplicities are lower in the hybrid model calculation due to the isentropic hydrodynamic expansion while the yields for strange particles are enhanced due to the local equilibrium in the hydrodynamic evolution. The elliptic flow values at SPS energies are shown to be in line with an ideal hydrodynamic evolution if a proper initial state is used and the final freeze-out proceeds gradually. The hybrid model calculation is able to reproduce the experimentally measured integrated as well as transverse momentum dependent $v_2$ values for charged particles. The multiplicity and mean transverse mass excitation function is calculated for pions, protons and kaons in the energy range from $E_{\rm lab}=2-160A~$GeV. It is observed that the different freeze-out procedures have almost as much influence on the mean transverse mass excitation function as the equation of state. The experimentally observed step-like behaviour of the mean transverse mass excitation function is only reproduced, if a first order phase transition with a large latent heat is applied or the EoS is effectively softened due to non-equilibrium effects in the hadronic transport calculation. The HBT correlation of the negatively charged pion source created in central Pb+Pb collisions at SPS energies are investigated with the hybrid model. It has been found that the latent heat influences the emission of particles visibly and hence the HBT radii of the pion source. The final hadronic interactions after the hydrodynamic freeze-out are very important for the HBT correlation since a large amount of collisions and decays still takes place during this period.
If we want to develop a semantic analysis for explicit performatives such as I promise you to free Willy, we are faced with the following puzzle: In order to account for the speech act expressed by the performative verb, one can assume that the so-called performative clause is purely performative and provides the illocutionary force of the speech act whose content is given by the semantic object denoted by the complement clause. Yet under this perspective, the performative clause that is, next to the performative verb, the indexicals I and you that refer to the speaker and to the addressee of the utterance context is semantically invisible and does not contribute compositionally its meaning to the meaning of the entire explicit performative sentence. Conversely, if we account for the truth conditional contribution of the performative clause and deny that the meaning of the performative verb is purely performative, then we have to find a way to account for the speech act expressed by the performative verb. Of course, there is already the widely accepted and very appealing indirectness account for explicit performative utterances developed by Bach & Harnish (1979). Roughly, Bach and Harnish solve this puzzle in deriving the performativity by means of a pragmatic inference process. According to them, the important speech act performed by means of the utterance of the explicit performative sentence is a kind of the conventionalized indirect speech act. However, the boundary between semantics and pragmatics can be drawn in many various ways. Therefore, I think there could be other perspectives regarding the interface between the truth-functional treatment of the declarative explicit performative sentences and the speech acts performed with their utterances and which are expressed by the performative verbs. Hence, this thesis consists in the experiment to develop a further analysis and to check out its consequences with respect to the semantics and pragmatics of explicit performative utterances and the new interface emerged. Briefly, the experiment runs as follows: First, I develop an analysis for explicit performative sentences framed by parenthetical structures such as in (1)(a). In a second step, this parenthetical analysis is applied to the proper Austinian explicit performative sentences in (1)(b). (1) a. Tomorrow, I promise you this, I will teach them Tyrolean songs. b. I promise you that I will teach them Tyrolean songs. To analyze at first explicit performatives framed by parenthetical structures bears the convenience that we are faced with two utterances of two main clauses. In (1)(a) there is the utterance of the host sentence Tomorrow I will teach them Tyrolean songs, and the utterance of the explicit parenthetical I promise you this, where the demonstrative this refers to the utterance of Tomorrow I will teach them Tyrolean songs. Since speakers perform speech acts with utterances of main clauses, I assume that the meaning of the explicit parenthetical I promise you this specifies that the actual illocutionary force of the utterance of Tomorrow I will teach them Tyrolean songs is the illocutionary force of a promise. Hence, instead of deriving an indirect illocutionary force by means of a pragmatic inference schema, we can deal with an ordinary direct speech act that is performed with the utterance of the host sentence. This kind of analysis stresses the particular discourse function of explicit performative utterances. Performative verbs are used whenever the contextual information is not sufficient to determine the illocutionary force of the corresponding implicit speech act. The resulting consequences of the parenthetical analysis are interesting since they cast a different light on performative verbs. Surprisingly, the performative verbs are not performative at all. They do not constitute the execution of a speech act, but are execution supporting. Instead of constituting the particular illocutionary force, they merely specify the illocutionary force of the utterance of the host sentence. For instance, the speaker utters the explicit parenthetical I promise you this for specifying what he is simultaneously doing. Hence the speaker does not succeed in performing the promise simply because he is uttering I promise you this. Rather, by means of the information conveyed by the utterance of I promise you this, the potential illocutionary forces of the utterance of the host sentence are disambiguated. Thus, it is not the case that explicit parentheticals are trivially true when uttered. Their function is more complex. Their self-verifying property (‘saying so makes it so’) is explained by means of disambiguation. Furthermore, according to the parenthetical analysis, instead of being purely performative, the performative verbs contribute compositionally their meanings to the truth conditions of the entire explicit performative sentence. Together with its consequences, this analysis is applied to the proper Austinian performatives, which display subordination. I assume that regardless of their structure, explicit performatives always semantically and pragmatically behave as the parenthetical analysis predicts.
This study addresses the structure-function relationships of three essential membrane proteins: Porin from Paracoccus denitrificans, Porin OmpG from Eschericia coli and BetP from Corynobacterium glutamicum using Fourier transform infrared (FT-IR) spectroscopy and Attenuated Total Reflection (ATR) techniques. The structure of porin from P. denitrificans is known for more than a decade; however, the mechanism for loss of functionality together with the monomerization was not clear. In this study we have addressed the role of lipids for the functionality of porin using FT-IR. OmpF porin was found to interact with the lipid molecules via the aromatic girdles surrounding the protein for functionality. In this study, molecular bonds and groups of the lipids were established as reporter groups probing at different depths of the bilayer in order to understand the interaction partner of the aromatic girdles of porins. Monomerization of the trimeric assembly of OmpF porin reconstituted in lipids is induced by increasing the temperature. Porin (OmpF) was found to be extremely stable: The secondary structure of the protein was unaltered up to the temperature-induced main transition, around 80-90 °C, above which it is denatured. However, the interaction of the aromatic girdle with the lipid molecules exhibited distinct changes at much lower temperature values (40 - 50°) where, according to the previous functional studies, monomerization and the loss of function occurs. The results are compared with OmpG porin from E.coli, for which the functional unit is a monomer. The aromatic girdle-lipid interaction was monitored by the tyrosine aromatic ring C=C vibrational mode, a universal marker for the protein stability and interaction. We have also found that the aromatic girdles of porins are interacting with the interfacial region of the lipid bilayer instead of lipid headgroups. Lipid-protein interaction was found to be not only essential for the structural stability, but also for the functionality of OmpF porin. We have also studied the structural properties of OmpG from E.coli. The structure of OmpG at two pH values has been resolved using X-ray crystallography and the channel has been proposed to attain different states at different pH values as closed (pH < 5.5) and open (pH >7.5). This study, using IR spectroscopy, revealed that the pH-induced opening and closing of the channel is reflected by the frequency shifts of the ? sheet structure. OmpG has more rigid ? barrel properties upon opening of the channel. IR spectral analysis revealed multiple ? sheet signals with different hydrogen bond strengths. This enabled us to monitor the formation of hydrogen bridges between the extracellular loops upon opening of the channel. The conclusion that OmpG porin having two states at different pH values was also confirmed by the three mutants where the role of the histidine pair (H231 & H261) and loop 6 has been addressed. Temperature-profiling of the wild type (WT) protein and the mutants did not show pH dependent structural stability differences in detergent solution. However, the WT protein was found to be more stable in the open form in 2D crystals than the closed form. Reconstitution into lipids has increased the transition temperature value by ~20 °C in the closed state and ~25 °C in the open state. Therefore we conclude that the open and closed state of OmpG has structural stability differences that are only revealed in the lipid environment. A comparison of the transition temperature values of OmpG WT and the mutants suggested that the hydrogen bond network among S218-H231-H261-D267, together with the formation of 12 residue-long ?-sheet contributes to the structural stability of the open channel. In the process of closing and opening of the channel, the globular structure of the protein remains mainly unchanged, while there are changes in the side chain moieties. In addition to the role of the histidine pair and the loop L6, in situ opening/closing experiments showed that the negatively charged amino acids, i.e. Asp and Glu, and Arg residues also play an active role; possibly by interacting with each other inside the pore lumen. Therefore it could be concluded that the closure of the channel at acidic pH values is not only via closing the channel entrance by loop 6, but also via changing the electric potential inside the lumen due to the different states of charged amino acids in order to effectively block the gateway. BetP from C.glutamicum attains an active and inactive state in order to adjust its glycine betaine uptake rate to the osmotic conditions that the cell encounters. The structure of BetP is not yet available. The WT protein exhibited structural differences in the presence of excess K+, which is one of the activation conditions. In 2D crystals, increasing the ionic strength to 700 mM K+ was shown to induce changes in the ?-helical moiety with contributions from the ester groups and one Tyr residue using ATR-FTIR. An increase in ionic strength to 220 mM K+ was found to be the threshold value of potassium concentration ([K+]) where the protein exhibits structural alterations in detergent solution. The determined [K+] values are in good agreement with the previous functional studies. However, there are differences in the activation profile of BetP in 2D crystals and in detergent solution, which points out that the lipids are involved in the conformational transition from the inactive to the active state and their absence can lead to different structural properties. BetP WT was found to have ~65% alpha-helix, ~25% random coil and ~10% turn structure in detergent solution. In the presence of excess K+, the WT protein is found to adapt more unordered structure. Secondary structure analysis of the mutants revealed that both the N- and C-terminus are in ?-helical conformation. Reconstitution of WT protein in 2D crystals increased the main transition (denaturation) temperature value from ~62 °C to ~85 °C, a clear indication that the protein is more stable in lipid environment. Temperature-profiling of the two forms of the WT protein revealed that the structural breakdown is preceeded by monomerization of the trimeric assembly. Comparing the two forms of the WT protein and the mutant BetA, we conclude that the oligomeric status is stabilized via the interactions among hydrophilic regions involving the N terminus. H/D exchange and activation with excess K+ in D2O-buffer revealed that activation of the protein involves the interaction of Arg and Asp/Glu residues in the cytoplasmic region of the protein. BetP WT and the two mutants tested, i.e. BetA and BetP?C45, showed differences in protein packing upon activation. The WT protein and BetP?C45 mutant also show changes in the hydrogen bonding properties of turns. Since BetA does not show such a property in activation, we conclude that the N-terminus interacts with the loops in the inactive state via the interaction of charged amino acids for the WT protein and that this interaction is altered during the activation. It could be argued that the protein packing is affected via the changes in turns upon activation. We also have found experimental evidence that one Tyr residue has different orientations in the active and inactive state of BetP. Based on the previous functional studies, it could be one of the five Tyr residues in the cytoplasmic region of the protein (in loop 3, 6, 7 or C-terminus). The mutant BetP?C45, on the other hand, showed fewer differences between the active and inactive state conditions and based on the H/D exchange rates, the mutant shows the properties of an active WT protein, proving that the C-terminal truncation impairs the conformational transition between the active and inactive states.
The characterization of microscopic properties in correlated low-dimensional materials is a challenging problem due to the effects of dimensionality and the interplay between the many different lattice and electronic degrees of freedom. Competition between these factors gives rise to interesting and exotic magnetic phenomena. An understanding of how these phenomena are driven by these degrees of freedom can be used for rational design of new materials, to control and manipulate these degrees of freedom in order to obtain desired properties. In this work, we study these effects in materials with small exchange interaction between the magnetic ions such as metal-organic and inorganic dilute compounds. We overcome the dfficulties in studying these kind of materials by combining classical and quantum mechanical ab initio methods and many-body theory methods in an effective theoretical approach. To treat metal-organic compounds we elaborate a novel two-step methodology which allows one to include quantum effects while reducing the computational cost. We show that our approach is an effective procedure, leading at each step, to additional insights into the essential features of the phenomena and materials under study. Our investigation is divided into two parts, the first one concerning the exploration of the fundamental physical properties of novel Cu(II) hydroquinone-based compounds. We have studied two representatives of this family, a polymeric system Cu(II)-2,5-bis(pyrazol-1-yl)-1,4-dihydroxybenzene (CuCCP) and a coupled system Cu2S2F6N8O12 (TK91). The second part concerns the study of magnetic phenomena associated with the interplay between different energy scales and dimensionality in zero-, one- and two-dimensional compounds. In the zero-dimensional case, we have performed a comprehensive study of Cu4OCl6L4 with L=diallylcyanamide=NC-N-(CH2-CH=CH2)2 (Cu4OCl6daca4). Interpretations of the magnetic properties for this tetrameric compound have been controversial and inconsistent. From our studies, we conclude that the common models usually applied to this and other representatives in the same family of cluster systems fail to provide a consistent description of their low temperature magnetic properties and we thus postulate that in such systems it is necessary to take into account quantum fluctuations due to possible frustrated behavior. In the one-dimensional case, we studied polymeric Fe(II)-triazole compounds, which are of special relevance due to the possibility of inducing a spin transition between low and high spin state by applying a external perturbation. A long standing problem has been a satisfactory microscopic explanation of this large cooperative phenomenon. A lack of X-ray data has been one mitigating reason for the absence of microscopic studies. In this work, we present a novel approach to the understanding of the microscopic mechanism of spin crossover in such systems and show that in these kind of compounds magnetic exchange between high spin Fe(II) centers plays an important role. The correct description of the underlying physics in many materials is often hindered by the presence of anisotropies. To illustrate this difficulty, we have studied a two dimensional dilute compound K2V3O8 which exhibits an unusual spin reorientation effect when applying magnetic fields. While this effect can be understood when considering anisotropies in the system, it is not sufficient to reproduce experimental observations. Based on our studies of the electronic and magnetic properties in this system, we predict an extra exchange interaction and the presence of an additional magnetic moment at the non-magnetic V site. This sheds a new light into the controversial recent experimental data for the magnetic properties of this material.
This thesis contributes to the field of soft matter research and studies the importance of hydrodynamic interactions during free-solution electrophoresis of linear polyelectrolytes by means of coarse-grained molecular dynamics simulations including full electro-hydrodynamic interactions. The center of attention is the specific role of hydrodynamic interactions on the electrophoretic behaviour of charged macromolecules. Points of interest are the dependence of hydrodynamic interactions on the chain length, the chain flexibility and the surrounding counterions, and their combined influence on important observables such as the static chain conformations and the dynamic transport coefficients, i.e., the diffusion and the electrophoretic mobility. These problems are addressed by extensive computer simulations that are quantitatively matched with experimental results. Existing theoretical predictions are carefully examined and are augmented by the observations in this thesis.